<p>This study describes the synthesis and comprehensive characterization of solid solutions in the <i>n</i> <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12039_2025_2363_Article_IEq3.gif" Format="GIF" Height="6" Rendition="HTML" Resolution="72" Type="Linedraw" Width="14" /> </InlineMediaObject> <EquationSource Format="TEX">\(=\)</EquationSource> <EquationSource Format="MATHML"><math> <mo>=</mo> </math></EquationSource> </InlineEquation> 3 and 4 members of the Dion–Jacobson (DJ) family of layered perovskites, <InlineEquation ID="IEq03"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12039_2025_2363_Article_IEq03.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="61" /> </InlineMediaObject> <EquationSource Format="TEX">\(\text{A}^\prime{\text{Ca}}_{2-x}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mtext>A</mtext> <mo>′</mo> </msup> <msub> <mtext>Ca</mtext> <mrow> <mn>2</mn> <mo>-</mo> <mi>x</mi> </mrow> </msub> </mrow> </math></EquationSource> </InlineEquation>Cd<sub><i>x</i></sub>Nb<sub>3</sub>O<sub>10</sub> and A′Ca<sub>2-<i>x</i></sub>Cd<sub><i>x</i></sub>NaNb<sub>4</sub>O<sub>13</sub> (A′ <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12039_2025_2363_Article_IEq4.gif" Format="GIF" Height="6" Rendition="HTML" Resolution="72" Type="Linedraw" Width="14" /> </InlineMediaObject> <EquationSource Format="TEX">\(=\)</EquationSource> <EquationSource Format="MATHML"><math> <mo>=</mo> </math></EquationSource> </InlineEquation> Rb, Cs) (0 ≤ <i>x</i> ≤ 2). In the <i>n</i> <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12039_2025_2363_Article_IEq5.gif" Format="GIF" Height="6" Rendition="HTML" Resolution="72" Type="Linedraw" Width="14" /> </InlineMediaObject> <EquationSource Format="TEX">\(=\)</EquationSource> <EquationSource Format="MATHML"><math> <mo>=</mo> </math></EquationSource> </InlineEquation> 3 series, both Rb and Cs oxides exhibit a transition from centrosymmetric (CS) towards non-centrosymmetric (NCS) polar structures (S.G. <i>Ima</i>2, <i>a</i><sub>O</sub> ~ 29.7 Å, <i>b</i><sub>O</sub> ~ 5.39 Å, <i>c</i><sub>O</sub> ~ 5.43 Å) from <i>x</i> <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12039_2025_2363_Article_IEq6.gif" Format="GIF" Height="6" Rendition="HTML" Resolution="72" Type="Linedraw" Width="14" /> </InlineMediaObject> <EquationSource Format="TEX">\(=\)</EquationSource> <EquationSource Format="MATHML"><math> <mo>=</mo> </math></EquationSource> </InlineEquation> 1 resembling <i>x</i> <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12039_2025_2363_Article_IEq7.gif" Format="GIF" Height="6" Rendition="HTML" Resolution="72" Type="Linedraw" Width="14" /> </InlineMediaObject> <EquationSource Format="TEX">\(=\)</EquationSource> <EquationSource Format="MATHML"><math> <mo>=</mo> </math></EquationSource> </InlineEquation> 2 phases, A′Cd<sub>2</sub>Nb<sub>3</sub>O<sub>10</sub> (A′ <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12039_2025_2363_Article_IEq8.gif" Format="GIF" Height="6" Rendition="HTML" Resolution="72" Type="Linedraw" Width="14" /> </InlineMediaObject> <EquationSource Format="TEX">\(=\)</EquationSource> <EquationSource Format="MATHML"><math> <mo>=</mo> </math></EquationSource> </InlineEquation> Rb, Cs). In the <i>n</i> <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12039_2025_2363_Article_IEq9.gif" Format="GIF" Height="6" Rendition="HTML" Resolution="72" Type="Linedraw" Width="14" /> </InlineMediaObject> <EquationSource Format="TEX">\(=\)</EquationSource> <EquationSource Format="MATHML"><math> <mo>=</mo> </math></EquationSource> </InlineEquation> 4 series, the transitions to acentric polar oxides occur for the Rb analogs (<i>x</i> ≥ 1.75). The polar RbCd<sub>2</sub>NaNb<sub>4</sub>O<sub>13</sub> (<i>n</i> <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12039_2025_2363_Article_IEq10.gif" Format="GIF" Height="6" Rendition="HTML" Resolution="72" Type="Linedraw" Width="14" /> </InlineMediaObject> <EquationSource Format="TEX">\(=\)</EquationSource> <EquationSource Format="MATHML"><math> <mo>=</mo> </math></EquationSource> </InlineEquation> 4) was confirmed through positive second harmonic generation and Le Bail refinements of the PXRD data. Structures of the Cs analogs and the rest of solid solution members including that for Rb adopt a CS tetragonal symmetry (S.G. <i>P</i>4/<i>mmm</i>, <i>a</i><sub>T</sub> ~ 3.9 Å; <i>c</i><sub>T</sub> ~ 18.9 Å), as demonstrated by the Rietveld refinements. Raman spectroscopy corroborates the local distortions of NbO<sub>6</sub> units. Estimation of the optical band gaps and valence and conduction bands energy levels illustrate their utilization for potential photocatalytic applications.</p> Graphical abstract <p>The colour wheel reveals the transition from centrosymmetric (CS) to non-centrosymmetric (NCS) structures based on the Cd content in the Dion-Jacobson (n <InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12039_2025_2363_Article_IEq12.gif" Format="GIF" Height="6" Rendition="HTML" Resolution="72" Type="Linedraw" Width="14" /> </InlineMediaObject> <EquationSource Format="TEX">\(=\)</EquationSource> <EquationSource Format="MATHML"><math> <mo>=</mo> </math></EquationSource> </InlineEquation> 3, 4) layered perovskite oxides, <InlineEquation ID="IEq031"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12039_2025_2363_Article_IEq031.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="61" /> </InlineMediaObject> <EquationSource Format="TEX">\(\text{A}^\prime{\text{Ca}}_{2-x}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mtext>A</mtext> <mo>′</mo> </msup> <msub> <mtext>Ca</mtext> <mrow> <mn>2</mn> <mo>-</mo> <mi>x</mi> </mrow> </msub> </mrow> </math></EquationSource> </InlineEquation>CdxNan-3NbnO3n+1 (A′ <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12039_2025_2363_Article_IEq11.gif" Format="GIF" Height="6" Rendition="HTML" Resolution="72" Type="Linedraw" Width="14" /> </InlineMediaObject> <EquationSource Format="TEX">\(=\)</EquationSource> <EquationSource Format="MATHML"><math> <mo>=</mo> </math></EquationSource> </InlineEquation> Rb, Cs; 0 ≤ x ≤ 2.0), forming a significant group of potential functional materials.</p>

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Structural distortions leading to potential polar materials in n \(=\) 3 and 4 Dion–Jacobson-layered perovskite series

  • Sachin Pal,
  • Sitharaman Uma

摘要

This study describes the synthesis and comprehensive characterization of solid solutions in the n \(=\) = 3 and 4 members of the Dion–Jacobson (DJ) family of layered perovskites, \(\text{A}^\prime{\text{Ca}}_{2-x}\) A Ca 2 - x CdxNb3O10 and A′Ca2-xCdxNaNb4O13 (A′ \(=\) = Rb, Cs) (0 ≤ x ≤ 2). In the n \(=\) = 3 series, both Rb and Cs oxides exhibit a transition from centrosymmetric (CS) towards non-centrosymmetric (NCS) polar structures (S.G. Ima2, aO ~ 29.7 Å, bO ~ 5.39 Å, cO ~ 5.43 Å) from x \(=\) = 1 resembling x \(=\) = 2 phases, A′Cd2Nb3O10 (A′ \(=\) = Rb, Cs). In the n \(=\) = 4 series, the transitions to acentric polar oxides occur for the Rb analogs (x ≥ 1.75). The polar RbCd2NaNb4O13 (n \(=\) = 4) was confirmed through positive second harmonic generation and Le Bail refinements of the PXRD data. Structures of the Cs analogs and the rest of solid solution members including that for Rb adopt a CS tetragonal symmetry (S.G. P4/mmm, aT ~ 3.9 Å; cT ~ 18.9 Å), as demonstrated by the Rietveld refinements. Raman spectroscopy corroborates the local distortions of NbO6 units. Estimation of the optical band gaps and valence and conduction bands energy levels illustrate their utilization for potential photocatalytic applications.

Graphical abstract

The colour wheel reveals the transition from centrosymmetric (CS) to non-centrosymmetric (NCS) structures based on the Cd content in the Dion-Jacobson (n \(=\) = 3, 4) layered perovskite oxides, \(\text{A}^\prime{\text{Ca}}_{2-x}\) A Ca 2 - x CdxNan-3NbnO3n+1 (A′ \(=\) = Rb, Cs; 0 ≤ x ≤ 2.0), forming a significant group of potential functional materials.